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NSR database version of April 11, 2024.

Search: Author = C.Y.Cheung

Found 12 matches.

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2005MI21      Nucl.Phys. A755, 571c (2005)

H.Mineo, S.N.Yang, C.Y.Cheung

Generalized parton distributions of the nucleon based on the Faddeev approach to the NJL model

doi: 10.1016/j.nuclphysa.2005.03.071
Citations: PlumX Metrics


2005MI24      Phys.Rev. C 72, 025202 (2005)

H.Mineo, S.N.Yang, C.-Y.Cheung, W.Bentz

Generalized parton distributions of the nucleon in the Nambu-Jona-Lasinio model based on the Faddeev approach

NUCLEAR STRUCTURE 1H; calculated spin-averaged and helicity-flip generalized parton distributions. Nambu-Jona-Lasinio model.

doi: 10.1103/PhysRevC.72.025202
Citations: PlumX Metrics


2000CH12      Nucl.Phys. A663-664, 667c (2000)

C.-Y.Cheung, W.-M.Zhang

Nonperturbative Determination of Heavy Meson Bound States

doi: 10.1016/S0375-9474(99)00710-1
Citations: PlumX Metrics


1991CH08      Nucl.Phys. A526, 674 (1991)

C.Y.Cheung, Y.S.Yeh

Compton Scattering by the Proton and Nucleon Polarizabilities

NUCLEAR REACTIONS 1H(γ, γ), E=low; calculated Compton scattering σ(θ), asymmetry; deduced nucleon polarizabilities role.

doi: 10.1016/0375-9474(91)90437-B
Citations: PlumX Metrics


1988MC03      Phys.Rev.Lett. 61, 814 (1988)

J.P.McDermott, E.Rost, J.R.Shepard, C.Y.Cheung

Relativistic (γ, p) Calculations at Intermediate Energies

NUCLEAR REACTIONS 16O(γ, p), E=196 MeV; 40Ca(γ, p), E=100-300 MeV; calculated σ(θ).

doi: 10.1103/PhysRevLett.61.814
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1988SH07      Phys.Rev. C37, 1130 (1988)

J.R.Shepard, E.Rost, C.-Y.Cheung, J.A.McNeil

Magnetic Response of Closed-Shell ±1 Nuclei in Dirac-Hartree Approximation

NUCLEAR REACTIONS 15N(e, e), E not given; calculated isoscalar M1 form factor. Dirac-Hartree approximation.

NUCLEAR STRUCTURE 15N, 15O; A=15, 17, 39, 41; calculated μ. Dirac-Hartree approximation.

doi: 10.1103/PhysRevC.37.1130
Citations: PlumX Metrics


1986CH05      Phys.Rev. C33, 776 (1986)

C.Y.Cheung, B.D.Keister

Role of the Δ(1232) in the (γ, p) Reaction

NUCLEAR REACTIONS 16O, 4He(γ, p), E=100-300 MeV; calculated σ(θ); deduced isobar role.

doi: 10.1103/PhysRevC.33.776
Citations: PlumX Metrics


1986MA21      Nucl.Phys. A454, 606 (1986)

O.V.Maxwell, C.Y.Cheung

Two-Body Absorption of Pions in 3He

NUCLEAR REACTIONS 3He(π+, 2p), (π-, np), E ≈ 20-180 MeV; calculated σ(E), σ(θ). 3He deduced σ(π+)/σ(π-). Two-body pion absorption, rescattering effects.

doi: 10.1016/0375-9474(86)90108-9
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1984CH32      Phys.Lett. 149B, 18 (1984)

C.Y.Cheung

Pion Effect in Deep-Inelastic Polarized-Lepton-Polarized-Nucleon Scattering

NUCLEAR REACTIONS 1H(polarized e, e'), E not given; calculated asymmetry; deduced nucleon quark spin polarization.

doi: 10.1016/0370-2693(84)91542-9
Citations: PlumX Metrics


1983CH25      Phys.Lett. 127B, 147 (1983)

C.Y.Cheung, R.M.Woloshyn

Electro-Disintegration of 2H with Polarized Beam and Target

NUCLEAR REACTIONS 2H(polarized e, e'n), (polarized e, e'X), E=1 GeV; calculated electrodisintegration σ(θ(e), θp) vs outgoing electron momentum, asymmetry vs θ; deduced neutron electric form factor dependence. Quasifree, fixed kinematics, longitudinal beam polarization, polarized target.

doi: 10.1016/0370-2693(83)90863-8
Citations: PlumX Metrics


1982CH27      Phys.Lett. 119B, 47 (1982)

C.Y.Cheung

Charge Symmetry and the Reaction d + d → 4He + π0

NUCLEAR REACTIONS 2H(d, π0), E=500-700 MeV; calculated σ(θ=0°). T-matrix approach, different charge symmetry breaking mechanisms.

doi: 10.1016/0370-2693(82)90240-4
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1980CH27      Nucl.Phys. A348, 365 (1980)

C.Y.Cheung, E.M.Henley, G.A.Miller

Charge Symmetry Breaking in the Neutron-Proton System

NUCLEAR REACTIONS 1H(n, n), E=160, 300 MeV; calculated polarization difference vs θ. 1H(n, d), E=577 MeV; calculated σ(θ). Charge symmetry breaking mechanism.

doi: 10.1016/0375-9474(80)90261-4
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